The Taylor expansions of $\sin$ and $\cos$ always converge, also when taking the explicit expansions in the point $0$. What they were referring to on the other page, is: when you only want to approximate, for example, $\sin(x)$, then you could use $$\sin(x)\approx x-\frac{x^3}{3!}+\frac{x^5}{5!}$$ since for small $x$, the terms after that are so small that they are negligible. But for large $x$, this isn't such a good approximation - however, the infinite sum $$\sin(x)=x-\frac{x^3}{3!}+\frac{x^5}{5!}-\cdots$$ still converges to the exact value for $\sin(x)$, no matter how big $x$ is.
Edit. If we take the Taylor expansion in another point than $0$, say, $2\pi$, then we get $$(x-2\pi)-\frac{(x-2\pi)^3}{3!}+\frac{(x-2\pi)^5}{5!}-\cdots$$ As we can see, taking only the first three terms would approximate $\sin(x)$ differently - it working better for values close to $2\pi$. This way we can intuitively see that yes, taking the Taylor expansion on another point
does influence the way $\sin(x)$ approximates $x$.